A Phosphorus Supported Multisite Coordinating Tris Hydrazone
P(S)[N(Me)NCHC6H4-o-OH]3 as an Efficient Ligand for the Assembly
of Trinuclear Metal Complexes: Synthesis, Structure, and Magnetism
posted on 2003-08-20, 00:00authored byVadapalli Chandrasekhar, Ramachandran Azhakar, Gurusamy Thanagavelu Senthil Andavan, Venkatasubbaiah Krishnan, Stefano Zacchini, Jamie F. Bickley, Alexander Steiner, Raymond J. Butcher, Paul Kögerler
A phosphorus supported multisite coordinating ligand P(S)[N(Me)NCHC6H4-o-OH]3 (2) was prepared by the
condensation of the phosphorus tris hydrazide P(S)[N(Me)NH2]3 (1) with o-hydroxybenzaldehyde. The reaction of
2 with M(OAc)2·xH2O (M = Mn, Co, Ni, x = 4; M = Zn, x = 2) afforded neutral trinuclear complexes
{P(S)[N(Me)NCHC6H4-o-O]3}2M3 [M = Mn (3), Co (4), Ni (5), and Zn (6)]. The X-ray crystal structures of
compounds 2−6 have been determined. The structures of 3−6 reveal that the trinculear metal assemblies are
nearly linear. The two terminal metal ions in a given assembly have an N3O3 ligand environment in a distorted
octahedral geometry while the central metal ion has an O6 ligand environment also in a slightly distorted octahedral
geometry. In all the complexes, ligand 2 coordinates to the metal ions through three imino nitrogens and three
phenolate oxygens; the latter act as bridging ligands to connect the terminal and central metal ions. The compounds
2−6 also show intermolecular CH···SP contacts in the solid-state which lead to the formation of polymeric
supramolecular architectures. The observed magnetic data for the (s = 5/2)3 L2(Mn(II))3 derivative, 3, show an
antiferromagnetic nearest- and next-nearest-neighbor exchange (J = −4.0 K and J‘ = −0.15 K; using the spin
Hamiltonian ĤHDvV = −2J(Ŝ1Ŝ2 + Ŝ2Ŝ3) − 2J‘Ŝ1Ŝ3). In contrast, the (s = 1)3 L2(Ni(II))3 derivative, 5, displays
ferromagnetic nearest-neighbor and antiferromagnetic next-nearest-neighbor exchange interactions (J = 4.43 K
and J‘ = −0.28 K; Ĥ = ĤHDvV+ Ŝ1DŜ1 + Ŝ2DŜ2+ Ŝ3DŜ3). The magnetic behavior of the L2(Co(II))3 derivative, 4,
reveals only antiferromagnetic exchange analogous to 3 (J = −4.5, J‘ = −1.4; same Hamiltonian as for 3).